Apparatus and method for evaluation of spectral properties of a measurement object

ABSTRACT

The invention relates to an apparatus and a method for evaluating spectral properties of a measurement object. It comprises a plurality of light emission units, each emitting light with a predetermined emission spectrum and having a respective output configured for emitting the light with the predetermined emission spectrum onto the measurement object, an optical spectrograph having an input port adapted to receive light from the measurement object and a diffraction unit adapted to distribute different wavelengths of the received light to different output ports comprising the optical detectors, wherein the diffraction unit is adapted to distribute said received light to the respective output ports such that the lights in the respective output port have different wavelengths at different diffraction orders; a signal identification unit adapted to identify which of the light emission units contribute to the respective light in the respective output ports.

FIELD

The invention relates to spectroscopy, and more particularly to anapparatus and a method using a spectrograph with a plurality of lightemission units operated sequentially or simultaneously to extend thespectral range of the spectrograph at a given spectral resolution.

BACKGROUND

One goal of optical spectroscopy is to determine the spectral content ofelectromagnetic radiation after it has interacted with some material orsample of interest. Typical wavelength dependent interactions includereflection, scattering and absorption and transmission.

Common instruments in the prior art fall into two general classes:spectrographs and spectrometers. A spectrograph disperses a spectrum inone step and records it using a multichannel optical detector, e.g. aphotodiode array or a CCD camera. A spectrometer, in contrast, scans thespectrum mechanically or electronically and records the responsesequentially using a single optical detector (D. W. Ball, “Field Guideto Spectroscopy”, SPIE Press, 2006).

Realizations of spectrographs typically comprise dispersive elements,e.g. prisms, reflection or transmission gratings, or arrayed waveguidegratings. Current realizations of spectrometers are usually based on thesuperposition of light, e.g. by using Michelson-, Fabry-Perot-, orMach-Zehnder couplers or interferometers.

Current advanced spectrometers can separate several 1000 channels with aspectral resolution in the order of 1 nm. Fourier transform infraredspectrometers (FT-IR) based on Michelson interferometers relax therequirements on the dimensions of the entrance slits and thereforeachieve higher output signals (Jacquinot principle). In order to furtherincrease the signal-to-noise ratio, multiple scans are employed(Fellgett principle). The spectral resolution, however, is related tothe optical path difference and thus to the span of the moving mirror.Thus, the mechanical stability and the reliability of high-resolutioninstruments represent an important cost-factor which restricts theapplication of FT-TR spectrometers to high-end laboratory equipment. Inaddition, due to the sequential measurement mode, they suffer frommeasurement periods in the order of minutes for high-resolution spectra.

The measurement period of spectrographs, in contrast, is only limited bythe response time of the multichannel optical detector and thesubsequent electronic circuitry. Many spectrographs are mechanicallyrobust since they do not exhibit any moving parts. Generally, theirspectral resolution is limited by the number of equally spacedwavelength channels. Although this is not a physical limit, shifting itcauses rapidly increasing technical difficulties and costs. Furthermore,compared to FT-IR spectrometers, spectrographs are more sensitive to thethermal noise of the detectors.

OBJECTS OF THE INVENTION

Therefore, the object of the present invention is to provide anapparatus and a method which circumvent the above describeddisadvantages, in particular measurement periods in the order of minutesfor FT-IR spectrometers and the limited spectral resolution ofconventional spectrographs.

SUMMARY OF THE DISCLOSURE

The invention according to one aspect provides an measurement apparatusfor evaluating spectral properties of a measurement object, comprising aplurality of light emission units, each emitting light with apredetermined emission spectrum and having a respective outputconfigured for emitting the light with the predetermined emissionspectrum onto the measurement object, an optical spectrograph having aninput port adapted to receive light from the measurement object and adiffraction unit adapted to distribute different wavelengths of receivedlight to different output ports comprising the optical detectors,wherein the diffraction unit is adapted to distribute said receivedlight to the respective output ports such that the lights in therespective output port have different wavelengths at differentdiffraction orders, and a signal identification unit adapted to identifywhich of the light emission units contribute to the respective light inthe respective output ports.

The invention according to another aspect provides a method forevaluating spectral properties of a measurement object, comprising thefollowing steps: emitting, by a plurality of light emission units,lights with predetermined emission spectra onto the measurement object,directing, the lights from the measurement object onto an opticalspectrograph, distributing, by an optical spectrograph having adiffraction unit, different wavelengths of the light received from themeasurement object to different output ports such that the lights in therespective output port have different wavelengths at differentdiffraction orders, and detecting, by optical detectors at the outputports, the lights, identifying, by a signal identification unit, whichof the light emission units contribute to the respective light in therespective output ports.

Briefly summarizing, the improvements listed under “SOLUTION OF THEINVENTION” for the solution of the single object listed under “OBJECT OFTHE INVENTION” let a N-channel spectrograph with K light emission unitsin fully simultaneous measurement mode work as an effective K*Nspectrograph. Advantages of the inventive device (and correspondinglythe method) are that it

-   -   has the same size as a spectrograph with N channels;    -   has the same measurement speed as a spectrograph with N        channels;    -   allows varying the channel positions and bandwidths over the        spectral range to match the requirements of the targeted        application;    -   offers an excellent signal-to-noise ratio;    -   is more cost-effective than conventional solutions as long as        the optical setup dominates the device cost;    -   and    -   is mechanically more robust than conventional solutions.

Further advantageous embodiments and improvements of the invention arelisted in the dependent claims. However, before coming to a detaileddescription of the embodiments of the invention with reference to thedrawings, hereinafter some more general further aspects of the inventionare considered.

According to a particularly advantageous aspect, the apparatus comprisesa control unit adapted to control the plurality of light emission unitsto emit light onto the measurement object sequentially in time. This hasthe particular advantage that the cost of electronic circuitry isminimized.

According to another aspect, the apparatus comprises a control unitadapted to control the plurality of light emission units to emit lightonto the measurement object simultaneously in time. This has the furtheradvantage that the measurement period is minimized.

According to another aspect, the signal identification unit is aN-channel heterodyne receiver. This has the further advantage that thecontrol unit and the signal identification unit are completelydecoupled.

According to another aspect, the apparatus comprises light emittingunits adapted to emit light in different wavelength ranges correspondingto the diffraction orders of the diffraction unit. This has the furtheradvantage of technical ease and of optimum use of the apparatus.Furthermore, this aspect allows the use of a single AWG (ArrayedWaveguide Grating) in different wavelength regions thus reducingmanufacturing costs.

According to yet another aspect, the diffraction unit can be an arrayedwaveguide grating. This has the further advantage that arrayed waveguidegratings can easily be operated in high diffraction orders.

According to another aspect, the light emitting units can be one or moreselected from the group consisting of a LED (Light Emitting Diode), anIRED (InfraRed Emitting Diode), a RCLED (Resonant Cavity Light EmittingDiode), an ELED (Edge Emitting LED), an SLED (Superluminescent LED), asemiconductor laser and a VCSEL (Vertical Cavity Surface EmittingLaser). This has the further advantage of using the optimal element withrespect to small footprint, low power consumption and low cost in everywavelength region.

According to another aspect, the light identification unit comprises aplurality of amplifiers. This has the further advantage that themeasurement period is minimized.

According to another aspect, the apparatus comprises one or moreamplifiers selected from the group consisting of lock-in amplifier,boxcar amplifier and correlator. This has the further advantage that thesignal-to-noise ratio is maximized.

According to another aspect, the light emitting units can emit light inthe near infrared region. This has the further advantage that theapparatus can be used for chemometrics.

According to a particularly advantageous aspect, in the above method,the light beams from the plurality of light emission units can beemitted onto the measurement object sequentially in time. This has theparticular advantage that the cost of electronic circuitry is minimized.

According to yet another aspect, in the above method, the lights fromthe plurality of light emission units are emitted onto the measurementobject simultaneously in time. This has the further advantage that themeasurement period is minimized.

According to another aspect, in the above method, the amplification isdone by using a lock-in amplifier. This has the further advantage thatthe signal-to-noise ratio is maximized.

According to another aspect, in the above method, the lights from theplurality of light emission units are emitted in different wavelengthranges corresponding to the diffraction orders of the diffraction unit.This has the further advantage that at least one part of the hardware ofthe apparatus is shared.

According to another aspect, in the above method, the lights of thelight emitting units are emitted in the near infrared region. This hasthe further advantage that the method can be used for chemometrics.

In addition, the invention according to another aspect provides anmeasurement apparatus for evaluating spectral properties of ameasurement object, comprising a light emission unit adapted to emitlight with a predetermined emission spectrum and having a respectiveoutput configured for emitting the light with the predetermined emissionspectrum onto the measurement object, an optical spectrograph having aninput port adapted to receive light from the measurement object and adiffraction unit adapted to distribute different wavelengths of thereceived light to different output ports comprising optical detectors,wherein the diffraction unit adapted to distribute said received lightto the respective output ports in different wavelengths and diffractionorders.

In addition, the invention according to yet another aspect provides amethod for evaluating spectral properties of a measurement object,comprising the following steps: emitting, by a light emission unit,light with a predetermined emission spectrum onto the measurementobject, directing), the light from the measurement object onto anoptical spectrograph, distributing, by the optical spectrograph having adiffraction unit, said received light to respective output ports of thespectrograph in different wavelengths and diffraction orders, detecting,by optical detectors at the output ports, the lights, identifying, by asignal identification unit the emitted light in the output ports.

Even when only one emission unit is used, the advantage of the inventivedevice and method is that it respectively

-   -   allows for channel positions of the emission unit in adjacent        diffraction orders;    -   offers an excellent signal-to-noise ratio;    -   is more cost-effective than conventional solutions as long as        the optical setup dominates the device cost; and    -   is mechanically more robust than conventional solutions.

Hereinafter, the invention will be described with reference to itsadvantageous embodiments with reference to the drawings. These drawings,where like reference numerals refer to identical or functionally similarelements throughout the separate views, together with the detaileddescription below, are incorporated in and form part of thespecification, and serve to further illustrate embodiments of conceptsthat include the claimed invention, and explain various principles andadvantages of those embodiments.

BRIEF DESCRIPTION OF THE DRAWINGS

In the drawings:

FIG. 1 is a block diagram of a first embodiment of the apparatusaccording to the invention;

FIG. 2 shows a realization of the apparatus using lock-in amplifiers;

FIG. 3 shows the parts of the N-channel detection unit;

FIG. 4 shows another realization of the apparatus of the invention usinglock-in amplifiers;

FIG. 5 shows a realization of the apparatus using N-channel heterodynedetection;

FIG. 6 shows the parts of a heterodyne detection unit used in theapparatus in FIG. 5;

FIG. 7 shows the spectra of the emission units and optimum mapping tothe corresponding diffraction orders (wavelengths not to scale of theapparatus according to the invention;

FIG. 8 shows an optical spectrograph based on an arrayed waveguidegrating according to the invention;

FIG. 9 shows arrangements of the emission units without (a) and withfiber pigtail, (b) and (c);

FIG. 10 shows a realization of the input unit 40 of the spectrograph forreflection measurements;

FIG. 11 shows a flow diagram of a first embodiment of the methodaccording to the invention;

FIG. 12 is a block diagram of a second embodiment of the methodaccording to the invention;

FIG. 13 shows a flow diagram of a further embodiment of the apparatusaccording to the invention; and

FIG. 14 illustrates the interdependence of wavelength and diffractionorder for an optical phased array.

Skilled artisans will appreciate that elements in the figures areillustrated for simplicity and clarity and have not necessarily beendrawn to scale. For example, the dimensions and locations of some of theelements in the figures may be exaggerated relative to other elements tohelp improve understanding of embodiments of the present invention. Thearrangement and method components have been represented whereappropriate by conventional symbols in the drawings, showing only thosespecific details that are pertinent to understanding the embodiments ofthe present invention so as not to obscure the disclosure with detailsthat will be readily apparent to those of ordinary skill in the arthaving the benefit of the description herein.

DETAILED DESCRIPTION

Briefly summarizing, as further explained below, the principle of thepresent invention is to extend the spectral range of a knownspectrograph at a given spectral resolution by using one or a pluralityof emission units with different emission spectra and by operating thespectrograph in a plurality of diffraction orders.

Before explaining the disclosed embodiments of the invention in detail,it is to be understood that the invention is not limited in itsapplication to the details of the particular arrangement, since theinvention is capable of other embodiments. Also, the terminology usedherein is for the purpose of description and not of limitation.

FIG. 1 shows a block diagram of an embodiment of the apparatus 100according to the invention for evaluating spectral properties of ameasurement object 1. As shown in FIG. 1, the apparatus 100 comprises aplurality of light emission units 2-1, 2-2, . . . 2-K each emittinglight with a predetermined emission spectrum and having a respectiveoutput configured for emitting the light with the predetermined emissionspectrum onto a measurement object 1. An optical spectrograph 3 has aninput port 40 adapted to receive light from the measurement object 1 anda diffraction unit 3-1 adapted to distribute different wavelengths ofthe received light to different output ports 41-1, 41-2, . . . 41-Ncomprising optical detectors. The light received from the measurementobject 1 may be transmitted or reflected light. Reference numeral 5designates a control unit for controlling the light emitting units, forexample to modulate them.

The diffraction unit 3-1 is adapted to distribute the received light tothe respective output ports 41-1, 41-2, . . . 41-N such that the lightsin the respective output port have different wavelengths at differentdiffraction orders. In embodiments of the present invention, K=2 and N=3(see the example below). Further preferably, for further typical workingexamples N=2 to 10 and K=8 to 128. However, it should be understood thatthe invention is by means limited to these numbers. Generally, N can begreater than K, N can be smaller than K or K can be equal to N,depending on the desired application. Hence, the number of N and K willdepend on the desired application.

The feature that the lights in the respective output port have differentwavelengths at different diffraction orders can be understood from thefollowing principles of physics. The interdependence between awavelength λ and a diffraction order m is governed by the gratingequationd _(in)+Λ sin θ=mλwhich dates back to J. Fraunhofer, “Kurzer Bericht von den Resultatenneuerer Versuche über die Gesetze des Lichtes and die Theoriederselben,” Ann. d. Phys. 74, 337-378 (1823). FIG. 14 illustrates theapplication to an arrayed waveguide grating. The diffraction region is aslab waveguide 3-10 in front of the output ports 41-1, 41-2, . . . 41-N,Λ is the grating constant and d_(in) is the optical path difference ofthe lights of adjacent incoming channel waveguides. The diffractionangle θ₄₁₋₁ designates the angle between the center and the output port41-1. Accordingly, the diffraction angles θ₄₁₋₁, θ₄₁₋₂, . . . θ_(41-N)point to the output ports 41-1, 41-2, . . . 41-N. For the diffractionorder m, lights with the wavelengths λ_(m,41-1), λ_(m,41-2), . . .λ_(m,41-N) will be directed to the output ports 41-1, 41-2, . . . 41-N.

For two different diffraction orders l and m, the wavelengths of thelights directed to the output ports 41-1, 41-2, . . . 41-N are thenrelated by the following equations which can be derived from the gratingequation, if the dispersion is neglected:lλ _(l,41-1) =mλ _(m,41-1)lλ _(l,41-2) =mλ _(m,41-2)lλ _(l,41-N) =mλ _(m,41-N)

These features let a N-channel spectrograph with K light emission unitsmapped to the diffraction orders work as an effective K*N spectrograph.The inventive apparatus advantageously uses spectrographs which can workin high diffraction orders such as arrayed waveguide gratings (AWGs). Ithas the same size as a spectrograph with N channels. The apparatus isclearly more cost-effective and also mechanically more robust thanconventional solutions.

A simple numerical example with K=2 light emission units and N=3 outputports illustrates the operation of the inventive apparatus. In thisexample, the center wavelength of the first light emission unit is 1500nm and the arrayed waveguide grating works in the 31^(st) diffractionorder for this light emission unit. The center wavelength of the secondlight emission unit is 1550 nm and the arrayed waveguide grating will,according to the above equations, work in the 30^(th) diffraction orderfor this light emission unit. If the spectral widths of the lightemission units are below 50 nm, light from the first emission unit willonly exist in 31^(st) diffraction order and light from the secondemission unit will only exist in 30^(st) diffraction order as shown inFIG. 7. If the arrayed waveguide grating is constructed such that thewavelengths assigned to the output ports 41-1, 41-2 and 41-3 are for thefirst emission unit 1480 nm, 1500 nm, 1520 nm, the wavelengths assignedto the output ports 41-1, 41-2 and 4-3 will, according to the aboveequations, be for the second emission unit 1529.3 nm, 1550 nm, 1570.6nm, i.e. the light at the output port 41-1 has a wavelength of 1480 nmfrom the or relating to the first emission unit and 1529.3 nm from theor relating to the second emission unit. Light at the output port 41-2has a wavelength of 1500 nm from the or relating to the first emissionunit and 1550 nm from the or relating to the second emission unit. Lightat the output port 41-3 has a wavelength of 1520 nm from the or relatingto the first emission unit and 1570.6 nm from the or relating to thesecond emission unit.

Hence, this example illustrates what is meant by “such that the lightsin the respective output port have different wavelengths at differentdiffraction orders”, namely that each output port has a lightcontribution from each light emission unit (in the above example each ofthe three output ports 41-1, 41-2, 41-3 has two lights (lightcontributions or light parts) from two light emission units). However,the light contributions per port are not in the same diffraction orderin the respective port (in the above example, the two lights in therespective output port are in the 31^(st) diffraction order (for thefirst emission unit) and in the 30^(th) diffraction order (for thesecond emission unit)). On the other hand, the different diffractionorders per output port are the same in each output port, that is eachoutput port has the light contribution from the first emission unit andthe second light emission unit in the same (different) diffractionorder, however, at respective different wavelengths. An AWG as describedhere as one embodiment of the diffraction unit 3-1 is capable ofproducing the light contributions at the respective output ports atdifferent wavelengths and in the different orders as just explained.Hence, whilst in classical spectroscopy higher order lights produced bygratings were considered as degradation and consequently were not used,in the present invention it is the particular desire to exploit and usethese higher order lights for spectroscopy.

The apparatus 100 in FIG. 1 further comprises a signal identificationunit 6 adapted to identify which of the light emission units contributeto the respective light in the respective output ports. This signalidentification unit 6 is provided for two reasons. Firstly, thesignal-to-noise ratio of the measured spectra can be improved if a lightemission unit is modulated. Secondly, by modulating the light emissionunits 2-1, 2-2, . . . 2-K individually, for example by the control unit5, it becomes possible to identify each single emission unit by ananalysis of the lights of the output ports 41-1, 41-2, . . . 41-N.Having the light emission units at the input modulated by the controlunit 5 thus allows the signal identification unit 6 at the output toidentify, when looking at the output light, the origin of the light,i.e. from which light emission unit the light stems.

The apparatus 100 including the N-channel spectrograph shown in FIG. 1preferably has a fully simultaneous measurement mode in which it worksas an effective K*N spectrograph. This has the advantage that at least apart of the hardware of the apparatus is shared.

With reference to FIG. 1, FIG. 11 shows an embodiment of the inventivemethod for evaluating spectral properties of the measurement object 1.As shown in FIG. 11, there is a first step S1 in which a plurality oflight emission units 2-1, 2-2, . . . 2-K emit lights with predeterminedemission spectra onto the measurement object 1. In a second step S2, thelights from the measurement object 1 are directed to the opticalspectrograph 3. In a further step S3 the optical spectrograph having adiffraction unit 3-1 of FIG. 1 distributes different wavelengths of thelight received (transmitted or reflected) from the measurement object 1to different output ports 41-1, 41-2, . . . 41-N such that the lights inthe respective output port have different wavelengths at differentdiffraction orders. In step S4 the optical detectors detect the lightsat the output ports 41-1, 41-2, . . . 41-N. In step S5, the signalidentification unit 6 identifies the lights from the light emissionunits 2-1, 2-2, . . . 2-K based on an analysis of the signals of theoutput ports 41-1, 41-2, . . . 41-N.

Although the high-priced part of the hardware of the apparatus 100 shownin FIG. 1—spectrograph and detector array—is shared between a pluralityof spectral ranges, the methodology allows an identification of thechannels controlled by the light emission units.

FIG. 2 shows a block diagram of the apparatus 100 comprising a controlunit 5 adapted to control the plurality of light emission units 2-1,2-2, . . . 2-K to emit light onto the measurement object 1 sequentiallyin time. This has the particular advantage that the cost of theapparatus is minimized.

The block diagram in FIG. 2 illustrates an embodiment based on lock-inamplifiers. The control unit 5 comprises an input port 50 to drive a 1:Kswitch 55 selecting the output ports 51-1, 51-2, . . . 51-K of thecontrol unit 5 driving the light emission units 2-1, 2-2, . . . 2-Ksequentially. The lock-in implementation further comprises a signalgenerator 53, the corresponding output port 52, and an amplifier 54.

The signal identification unit 6 can comprise an N-channel detectionunit 7, as shown in detail in FIG. 3. An input port 60 for a referencesignal is connected to the corresponding port 52 of the control unit 5.The analog input port of the N-channel detection unit 7 is, afterpre-amplification using amplifiers 63-1, 63-2, . . . 63-N, connected tothe corresponding output ports 61-1, 61-2, . . . 61-N of the signalidentification unit 6. The N-channel detection unit 7 is connected tothe digital output ports 62-1, 62-2, . . . 62-N.

FIG. 3 shows further details of the N-channel detection unit 7 used inthe implementations described in FIG. 2 and FIG. 4. Reference numeral 70designates an input port for the reference signal, reference numerals71-1, 71-2, . . . 71-N designate the analog input ports of the N-channeldetection unit, reference numerals 72-1, 72-2, . . . 72-N designate thedigital output ports. Reference numeral 73 designates a delay element,reference numerals 74-1, 74-2, . . . 74-N designate mixers. Referencenumerals 75-1, 75-2, . . . 75-N designate low-pass filters and referencenumerals 76-1, 76-2, . . . 76-N designate analog-to-digital converters.Optional electronic functions such as bandpass filters, notch filters,analog signal compressors, e.g. logarithmic amplifiers, automatic gaincontrol or range switching, and output amplifiers are not shown.

As a modification of the of the N-channel detection unit according toFIG. 3, the single delay element 73 shown in FIG. 3, can be replaced byN individually tunable delay elements, each one located in an input linein front of a mixer 74-1, 74-2, . . . 74-N. Such a setup is useful fortime-resolved measurements.

FIG. 4 shows another embodiment of the apparatus 100, comprising acontrol unit 5 adapted to control the plurality of light emission units2-1, 2-2, . . . 2-K to emit light onto the measurement object 1simultaneously in time. It also illustrates an aspect of the methodaccording to the invention, wherein the lights from the plurality oflight emission units 2-2, 2-1, . . . 2-K are emitted onto themeasurement object 1 simultaneously in time.

FIG. 4 shows a specific embodiment of the invention based on lock-inamplifiers. In this embodiment, the control unit 5 comprises outputports 51-1, 51-2, . . . 51-K driving the light emission units 2-1, 2-2,. . . 2-K simultaneously by using signal generators 53-1, 53-2, . . .53-K amplified separately by the amplifiers 54-1, 54-2, . . . 54-K, andoutput ports for reference signals 52-1, 52-2, . . . 52-K.

In FIG. 4, the signal identification unit 6 can comprise K N-channeldetection units 7-1, 7-2, . . . 7-K whose input ports for the referencesignals 60-1, 60-2, . . . 60-K are connected to the corresponding ports52-1, 52-2, . . . 52-K. After pre-amplification using the amplifiers63-1, 63-2, . . . 63-N, the analog input ports 71-1, 71-2, . . . 71-N ofthe N-channel detection units 7-1, 7-2, . . . 7-K are connected to thecorresponding ports 61-1, 61-2, . . . 61-N of the signal identificationunit 6. Each of the N-channel detection units 7-1, 7-2, . . . 7-K hasseparate digital output ports, i.e. the N-channel detection unit k isconnected to the digital output ports 62-k-1, 62-k-2, . . . 62-k-N wherek is any number between 1 and K.

FIG. 5 shows a further embodiment of the apparatus of the invention. InFIG. 5 the apparatus 200 EINZEICHNEN includes a control unit 5comprising output ports 51-1, 51-2, . . . , 51-K driving the lightemission units 2-1, 2-2, . . . 2-K simultaneously by using signalgenerators 53-1, 53-2, . . . 53-K amplified separately by the amplifiers54-1, 54-2, . . . 54-K. The signal identification unit 6 comprises aplurality of heterodyne detection units 8-1, 8-2, . . . 8-N connected tothe corresponding ports 61-1, 61-2, . . . 61-N of the signalidentification unit 6. The heterodyne detection units 8-1, 8-2, . . .8-N share a local oscillator 64 which can be tuned via port 65. Oneadvantage of the configuration according to FIG. 5 is that the controlunit 5 and the signal identification unit 6 are completely decoupled.

FIG. 6 shows a standard realization of the heterodyne detection unit 8used in the implementation shown in FIG. 5. In FIG. 6, reference numeral80 designates the input port of the reference from the local oscillator64, numeral 81 the input port from the signals emitted from one of thelight emission units 2-1, 2-2, . . . 2-K. The signal from port 81 isfirst filtered by a “radio” frequency RF band-pass filter 83, i.e. thesignal used by one of the signal generators 53-1, 53-2, . . . 53-K inthe control unit 5. The dotted line indicates that the local oscillatorand RF filter 83 are tuned in tandem. Next the signal passes the RFamplifier 84. The frequency mixer 85 carries out the actualheterodyning, i.e. it changes the incoming radio frequency signal to afixed intermediate frequency IF. The signal then passes the IF band-passfilter 86, the optional IF amplifier 87, and the demodulator 88.

FIG. 7 shows preferred spectra of the emission units and optimal mappingto the corresponding diffraction orders in the embodiments of theinvention. Wavelengths are not to scale. In particular, in order toallow the lights to be distributed by the diffraction unit to thedifferent output ports such that the lights in the respective outputport have different wavelengths at different diffraction orders, eachlight emitting unit 2-1, 2-2 . . . 2-K has a spectral widthsubstantially limited to the respective diffraction order m, m−1 . . .m−K+1 wavelength.

FIG. 8 shows an embodiment of the apparatus of the invention where thediffraction unit 3-1 is an arrayed waveguide grating (AWG). Thediffraction region is a slab waveguide 3-10 in front of the output ports41-1, 41-2, . . . 41-N. Arrayed waveguide gratings are optimized foroperation in high diffraction order.

In general, the light emitting units 2-1, 2-2, . . . 2-K can be selectedfrom the group consisting of an LED, an IRED, a RCLED, an ELED, an SLED,a semiconductor laser and a VCSEL which offer a plurality of advantagesincluding the option to transmit required signals to the signalidentification unit, to provide an emission spectrum compatible with thespectrograph, and to offer small size and low power consumption comparedto usual broadband emission units.

FIG. 9 shows optional arrangements of the emission units 2: withoutfiber pigtail in FIG. 9a and with fiber pigtail in FIG. 9b and FIG. 9c .According to FIG. 9a , the apparatus can comprise a light emitting unit2 comprising a lens 20 for collimating the lights of the light emissionunits 2-1, 2-2, . . . 2-K and directing them to the measurement object1. According to FIG. 9b , the apparatus can comprise a light emittingunit 2 comprising a lens 20 coupling the lights of light emission units2-1, 2-2, . . . 2-K into an optical fiber 21 and directing them via asecond lens to the measurement object 1. According to FIG. 9c a setupcan be used where the lights of the emission units 2-1, 2-2, . . . 2-Kof the light emitting unit 2 are separately coupled to optical fiberswhich in turn are coupled into a single optical fiber 21 using anoptical multiplexer 22 and then directed via a second lens 20 to themeasurement object 1. Arrangements with fiber pigtail are preferred wheneither the access to the measurement object 1 is complicated ormeasurements are done in an explosive environment.

For the arrangements according to FIGS. 9b and 9c , any kind ofsingle-mode and multimode fibers can be used and best practice is toadapt the fiber type to the requirements of the spectrograph.

FIG. 10 shows an embodiment of the input unit 40 of the spectrograph forreflection measurements shown in FIG. 1. It can comprise a collimationlens 401 coupling the lights into a fiber 402. An optical multiplexer403 combines the lights of the emission units 2-1, 2-2, . . . 2-Kaccording to FIG. 9b or 9 c and the optical spectrograph 3. The opticalpath between optical multiplexer 403 and the measurement object 1 has toprovide a high return loss to prevent light from traveling back.Arrangements with fiber pigtail are preferred when either the access tothe measurement object is complicated or measurements are done in anexplosive environment.

FIG. 12 shows a block diagram of a second embodiment of the apparatusaccording to the invention for evaluating spectral properties of ameasurement object 1. As shown in FIG. 12, it comprises a single lightemission unit 2′ adapted to emit light with a predetermined emissionspectrum and having a respective output configured for emitting thelight with the predetermined emission spectrum onto the measurementobject 1. An optical spectrograph 3 has an input port 40 adapted toreceive light from the measurement object 1 and a diffraction unit 3-1adapted to distribute different wavelengths of the received light todifferent output ports 41-1, 41-2, . . . 41-N comprising the opticaldetectors. The diffraction unit 3-1 distributes said received light tothe respective output ports 41-1, 41-2, . . . 41-N in differentwavelengths and diffraction orders. The light received from themeasurement object 1 may be transmitted or reflected light.

With reference to FIG. 12, FIG. 13 shows a second embodiment of theinventive method for evaluating spectral properties of the measurementobject 1. As shown in FIG. 13, there is a first step S1 in which asingle light emission unit 2′ emits light with a predetermined emissionspectrum onto the measurement object 1. In a second step S2, the lightfrom the measurement object 1 is directed onto an optical spectrograph3. In a further step S3, the optical spectrograph 3 having a diffractionunit 3-1 of FIG. 12 distributes different wavelengths of the lightreceived from the measurement object 1 to different output ports 41-1,41-2, . . . 41-N such that the lights in the respective output port havedifferent wavelengths at different diffraction orders. In step S4, theoptical detectors detect the lights at the output ports 41-1, 41-2, . .. 41-N. In step S5, the signal identification unit 6 identifies thelights from the light emission units 2-1, 2-2, . . . 2-K based on ananalysis of the signals of the output ports 41-1, 41-2, . . . 41-N.

The N-channel spectrograph shown in FIG. 11 preferably has only oneemission unit.

Even, when only one emission unit is used as in the second embodiment,it still allows for channel positions of the emission unit in adjacentdiffraction orders, i.e. the emission unit must not perfectly match thediffraction orders of the spectrograph.

From the current point of view, near-infrared spectroscopy is the mostattractive application of the invention which can use light-emittingdiodes LEDs in the NIR wavelength region. Such elements are availablefrom several suppliers like Hamamatsu www.hamamatsu.com or LEDMicrosensor NT (www.lmsnt.com). For use in the UV, visible or IRwavelength regions, LEDs are available from suppliers like Nichia(www.nichia.co.jp), OSRAM (www.osram.com/cb/index.jsp), CRE E(www.cree.com/led-chips/products) or LED Microsensor NT (lmsnt.com/).Photodiodes in the NIR and IR regions, usable for the invention, areavailable in the market, e.g. from Hamamatsu (www.hamamatsu.com), LASERCOMPONENTS (www.lasercomponents.com) or LED Microsensor NT lmsnt.com,Furthermore, for use in the invention, photodiodes for UV and visibleapplications based on Si and optimized for a special wavelength rangeare available from LASER COMPONENTS (www.lasercomponents.com).

Arrayed waveguide gratings, usable in the invention, are available fromNTT Electronics (www.ntt-electronics.com) including devices with channelspacings of 25-200 GHz corresponding to 0.2-1.6 nm at 1550 nm andbetween 8 and 128 wavelength channels.

The invention may use lock-in amplifiers, boxcar amplifiers orcorrelators available as stand-alone devices, which have been availablefor many years. They may be used to serve as the signal identificationunit as a system on chip (SoC).

One target application of the invention is spectroscopy. Thenear-infrared spectroscopy of the invention using the near-infraredregion of the electromagnetic spectrum from 780 nm to 2500 nm isparticularly useful for chemometrics including pharmaceutical, food andagrochemical quality control as well as for medical and physiologicaldiagnostics and Mid-infrared spectroscopy from 2500 nm to 25000 nm. Dueto its small size, low weight and fast processing speed the apparatus ofthe invention can be used advantageously as a small portable testingdevice for ad hoc tests of pharmaceutical substances such that thesubstances can be tested on site without the need to send samplesthereof to an analysis lab, saving costs and time.

In the foregoing specification, specific embodiments have beendescribed. However, one of ordinary skill in the art appreciates thatvarious modifications and changes can be made without departing from thescope of the invention as set forth in the claims below. Accordingly,the specification and figures are to be regarded in an illustrativerather than a restrictive sense, and all such modifications are intendedto be included within the scope of present teachings.

The benefits, advantages, solutions to problems, and any element(s) thatmay cause any benefit, advantage, or solution to occur or become morepronounced are not to be construed as a critical, required, or essentialfeature or element of any or all the claims. The invention is definedsolely by the appended claims including any amendments made during thependency of this application and all equivalents of those claims asissued.

Moreover, in this document, relational terms such as first and second,top and bottom, and the like may be used solely to distinguish oneentity or action from another entity or action without necessarilyrequiring or implying any actual such relationship or order between suchentities or actions. The terms “comprises”, “comprising”, “has”,“having”, “includes”, “including”, “contains”, “containing”, or anyother variation thereof, are intended to cover a non-exclusiveinclusion, such that a process, method, article, or apparatus thatcomprises, has, includes, contains a list of elements does not includeonly those elements, but may include other elements not expressly listedor inherent to such process, method, article, or apparatus. An elementproceeded by “comprises . . . a”, “has . . . a”, “includes . . . a”, or“contains . . . a”, does not, without more constraints, preclude theexistence of additional identical elements in the process, method,article, or apparatus that comprises, has, includes, or contains theelement. The terms “a” and “an” are defined as one or more unlessexplicitly stated otherwise herein. The terms “substantially”,“essentially”, “approximately”, “about”, or any other version thereof,are defined as being close to as understood by one of ordinary skill inthe art, and in one non-limiting embodiment the term is defined to bewithin 10%, in another embodiment within 5%, in another embodimentwithin 1%, and in another embodiment within 0.5%. The term “coupled” asused herein is defined as connected, although not necessarily directlyand not necessarily mechanically. A device or structure that is“configured” in a certain way is configured in at least that way, butmay also be configured in ways that are not listed.

It will be appreciated that some embodiments may be comprised of one ormore generic or specialized processors (or “processing devices”) such asmicroprocessors, digital signal processors, customized processors, andfield programmable gate arrays (FPGAs), and unique stored programinstructions (including both software and firmware) that control the oneor more processors to implement, in conjunction with certainnon-processor circuits, some, most, or all of the functions of themethod and/or apparatus described herein. Alternatively, some or allfunctions could be implemented by a state machine that has no storedprogram instructions, or in one or more application specific integratedcircuits (ASICs), in which each function or some combinations of certainfunctions are implemented as custom logic. Of course, a combination ofthe two approaches could be used.

Software programs containing software instructions for carrying out thefunctionalities and method steps in the described units may be used.Therefore, one or more embodiments can be implemented as acomputer-readable storage medium having computer readable code storedthereon for programming a computer (e.g., comprising a processor) toperform a method as described and claimed herein. Examples of suchcomputer-readable storage mediums include, but are not limited to, ahard disk, a CD-ROM, an optical storage device, a magnetic storagedevice, a ROM (Read Only Memory), a PROM (Programmable Read OnlyMemory), an EPROM (Erasable Programmable Read Only Memory), an EEPROM(Electrically Erasable Programmable Read Only Memory) and a Flashmemory. Further, it is expected that one of ordinary skill,notwithstanding possibly significant effort and many design choicesmotivated by, for example, available time, current technology, andeconomic considerations, when guided by the concepts and principlesdisclosed herein, will be readily capable of generating such softwareinstructions and programs and ICs with minimal experimentation.

The Abstract of the Disclosure is provided to allow the reader toquickly ascertain the nature of the technical disclosure. It issubmitted with the understanding that it will not be used to interpretor limit the scope or meaning of the claims.

In addition, in the foregoing description it can be seen that variousfeatures are grouped together in various embodiments for the purpose ofstreamlining the disclosure. This method of disclosure is not to beinterpreted as reflecting an intention that the claimed embodimentsrequire more features than are expressly recited in each claim. Rather,as the following claims reflect, inventive subject matter lies in lessthan all features of a single disclosed embodiment. Thus, the followingclaims are hereby incorporated into the description, with each claimstanding on its own as a separately claimed subject matter.

-   1 measurement object-   2 arrangement of the light emission units-   2′ light emission unit-   2-1, 2-2, . . . 2-K light emission units-   20 lens used in an arrangement of the light emission units-   21 optical fiber used in an arrangement of the light emission units-   22 optical fiber multiplexer used in an arrangement of the light    emission units-   3 optical spectrograph-   3-1 diffraction unit-   40 input port of the optical spectrograph-   41-1, 41-2, . . . 41-N output ports of the optical spectrograph    comprising optical detectors-   5 control unit of the light emission units-   50 input port of the control unit driving the 1:K switch-   51-1, 51-2, . . . 51-K output ports of the control unit driving the    light emission units-   52-1, 52-2, . . . 52-K output ports of the control unit providing    the reference signals-   53-1, 53-2, . . . 53-K signal generators-   54-1, 54-2, . . . 54-K amplifiers for the signal generators-   6 signal identification unit-   60 single input port of the signal identification unit for the    reference signal-   60-1, 60-2, . . . 60-K multiple input ports of the signal    identification unit for the reference signal-   61-1, 61-2, . . . 61-N input ports of the signal identification unit    for the output ports of the spectrograph-   62-1, 62-2, . . . 62-N output ports of the signal identification    unit assigned to the output ports of the spectrograph-   62-k-1, 62-k-2, . . . 62-k-N output ports of the signal    identification unit assigned to the output ports of the spectrograph    and the emission unit k-   63-1, 63-2, . . . 63-N preamplifiers for the signals from the    detectors-   64 local oscillator-   7 N-channel detection unit-   7-1, 7-2, . . . 7-N multiple N-channel detection units-   70 input port for the reference signal of a N-channel detection unit-   71-1, 71-2, . . . 71-N analog input ports of a N-channel detection    unit-   72-1, 72-2, . . . 72-N digital output ports of a N-channel detection    unit-   73 delay element of a N-channel detection unit-   74-1, 74-2, . . . 74-N mixers of a N-channel detection unit-   75-1, 75-2, . . . 75-N low-pass filters of a N-channel detection    unit-   76-1, 76-2, . . . 76-N analog-to-digital converters of a N-channel    detection unit-   8 heterodyne detection unit-   8-1, 8-2, . . . 8-N multiple heterodyne detection units-   80 input port for the reference from the local oscillator-   81 input port for the signal from one detector-   82 output port of a heterodyne detection unit-   83 radio frequency (RF) band-pass filter-   84 amplifier for the signal from one detector-   85 frequency mixer-   86 intermediate frequency (IF) band-pass filter-   87 amplifier for an intermediate frequency (IF) signal

The invention claimed is:
 1. A measurement apparatus (100) forevaluating spectral properties of a measurement object (1); comprising:a plurality of light emission units (2-1, 2-2, . . . 2-K), each emittinglight with a predetermined emission spectrum and having a respectiveoutput configured for emitting the light with the predetermined emissionspectrum onto the measurement object (1); an optical spectrograph (3)having an input port (40) adapted to receive light from the measurementobject (1) and a diffraction unit (3-1) adapted to distribute differentwavelengths of the received light to different output ports (41-1, 41-2,. . . 41-N) comprising optical detectors; the diffraction unit (3-1)adapted to distribute said received light to the respective output ports(41-1, 41-2, . . . 41-N) such that the lights in the respective outputport have different wavelengths at different diffraction orders; and asignal identification unit (6) adapted to identify which of the lightemission units contribute to the respective light in the respectiveoutput ports.
 2. The apparatus according to claim 1, further comprisinga control unit (5) adapted to control the plurality of light emissionunits (2-1, 2-2, . . . 2-K) to emit light onto the measurement object(1) sequentially in time.
 3. The apparatus according to claim 2, furthercomprising a control unit (5) adapted to control the plurality of lightemission units (2-1, 2-2, . . . 2-K) to emit light onto the measurementobject (1) simultaneously in time.
 4. The apparatus according to claim1, further comprising a control unit (5) adapted to control theplurality of light emission units (2-1, 2-2, . . . 2-K) to emit lightonto the measurement object (1) simultaneously in time.
 5. The apparatusaccording to claim 1, wherein the signal identification unit (6) is aN-channel heterodyne receiver.
 6. The apparatus according to claim 1,wherein the light emitting units (2-1, 2-2, . . . 2-K) are adapted toemit light in respectively different wavelength ranges corresponding tothe diffraction orders of the diffraction unit.
 7. The apparatusaccording to claim 1, wherein said diffraction unit (3-1) is an arrayedwaveguide grating.
 8. The apparatus according to claim 1, wherein saidlight emitting units (2-1, 2-2, . . . 2-K) are one or more selected fromthe group consisting of a pumped broadband fiber source, a LED, a RED, aRCLED, a ELED, a SLED, a semiconductor laser and a VCSEL.
 9. Theapparatus according to claim 1, wherein said light identification unit(6) comprises a plurality of amplifiers.
 10. The apparatus according toclaim 9, wherein said amplifiers comprise one or more selected from thegroup consisting of a lock-in amplifier, a boxcar amplifier and acorrelator.
 11. The apparatus according to claim 1, wherein said lightemitting units (2-1, 2-2, . . . 2-K) emit light in the near infraredregion.
 12. The method according to claim 1, wherein the lights of thelight emitting units (2-1, 2-2, . . . 2-K) are in the near infraredregion.
 13. The method according to claim 1, wherein the lights of thelight emitting units (2-1, 2-2, . . . 2-K) are in the near infraredregion.
 14. A method for evaluating spectral properties of a measurementobject (1), comprising the following steps emitting (S1), by a pluralityof light emission units (2-1, 2-2, . . . 2-K), lights with predeterminedemission spectra onto the measurement object (1); directing (S2), thelights from the measurement object (1) onto an optical spectrograph (3);distributing (S3), by the optical spectrograph (3) having a diffractionunit (3-1), different wavelengths of the light received from themeasurement object (1) to different output ports (41-1, 41-2, . . .41-N) such that the lights in the respective output port have differentwavelengths at different diffraction orders; and detecting (S4), byoptical detectors at the output ports (41-1, 41-2, . . . 41-N), thelights; and identifying (S5), by a signal identification unit (6), whichof the light emission units contribute to the respective light in therespective output ports.
 15. The method according to claim 14, whereinthe lights from the plurality of light emission units (2-2, 2-1, . . .2-K) are emitted onto the measurement object (1) sequentially in time.16. The method according to claim 14, wherein the lights from theplurality of light emission units (2-1, 2-2, . . . 2-K) is emitted ontothe measurement object (1) simultaneously in time.
 17. The methodaccording to claim 14, wherein said identifying step comprisesamplifying output signals of the optical detectors, wherein theamplification is done by using a lock-in amplifier.
 18. The methodaccording to claim 14, wherein the lights from the plurality of lightemission units (2-1, 2-2, . . . 2-K) are emitted in different wavelengthranges corresponding to the diffraction orders of the diffraction unit(3-1).